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XPCS at the APS: Implementation and Operations
Alec Sandy
X-Ray Science Division
Argonne National Laboratory
2
Acknowledgements
Sector Staff
– Suresh Narayanan
– Michael Sprung
TRR Group Leader
– Jin Wang
Former CAT members and continuing active partners:
– Larry Lurio
– Simon Mochrie
– Mark Sutton
3
Outline
Background
Mission
Implementation
Scientific and General User Program
Opportunities for Improvement (at NSLS-II)
Challenges
4
Background
Sector 8-ID
– ≤ 2002 IMM-CAT• IBM, McGill and MIT• Multiple experiment capabilities promised in PDR but not delivered
because of costs and dwindling PI participation – Beamline specialization a hidden benefit
– One of first 3 CAT’s designated by DOE for transition to APS operational responsibility
– 2003–current• Transition to APS XOR operations completed
– IMMY/XOR CAT → XOR 8-ID– Beamline staffed with APS personnel within the Time Resolved
Research Group– Beamtime allocated via APS General/Partner User system– Capital and operational funds via APS
5
Mission
Beamline Mission
– Develop and apply X-Ray Photon Correlation Spectroscopy (XPCS) to the study of equilibrium and non-equilibrium dynamics in condensed matter
• Small Q XPCS (Station 8-ID-I)• (Limited) Large Q XPCS, liquid surface XPCS (Station 8-ID-E)
– Currently, one of 2 such facilities in the world
– Develop and apply Grazing Incidence Small-Angle X-Ray Scattering (GISAXS) to study the structure and ordering kinetics of thin films (8-ID-E)
– “High-end” SAXS (Station 8-ID-I)
– Coherent diffraction imaging (Station 8-ID-I)
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Implementation
Beamline 8-ID is a minimalist undulator beamline
– Minimal optics for coherence preservation
– Minimal diagnostics because of legacy cost considerations
– First and second optics enclosures: 8-ID-A and 8-ID-D
– Experiment stations: 8-ID-E and 8-ID-I Primary features
– Simultaneous experiment operations in 8-ID-E and 8-ID-I via beam-splitting monochromator in 8-ID-D
– Pinhole and mirror in 8-ID-A to reduce downstream power load
Undulator A
8-ID-A FOE
8-ID-D
8-ID-E
8-ID-IMono or Pink beam
0 m
30 m51 m
65 m
GISAXS
Small-angle XPCS
Mono beam
“G”“E”
large Q XPCS
7
Implementation
8-ID (ongoing) design requirements
– Preserve delivered coherence
– Provide extremely stable and reproducible coherent x-ray beam to experimenters
– (Fully utilize delivered coherence)
Requirements achieved by
– Minimizing number of optical components
– Minimizing power loading
– (Implementing vertical focusing)
8
Implementation
Radiation Source
– High beta straight section
– 1-σ source sizes (σ) 270 m (H) × 9 m (V)
– 1× Undulator A (72-pole by 3.3 cm = 2.4 m device in 5 m straight) Transverse Coherence Lengths
– ξ = λR/(2πσ) → 7 m (H) × 200 m (V)
– Low-beta [σ = 120 m (H)] operations possible and will be examined during upcoming operations cycles
5 m straight section allows tandem undulator in the future
2X Undulator
8-ID-A FOE
8-ID-D
8-ID-E
8-ID-IMono or Pink beam
0 m
30 m51 m
65 m GISAXS,large Q XPCS
Small-angle XPCS
Monobeam
9
Implementation
First Optics Enclosure 8-ID-A
– Windowless connection to APS front end• Used by 40% of APS ID beamlines with no operational issues over
past 10 years• Preserves beam brilliance
PINHOLE APERTURE and DIFFERENTIAL PUMP
– Pinhole aperture• 300 m exit diameter tapered
pinhole greatly reduces transmitted power without sacrificing useful coherent flux– Incident power 1600 watts,
transmitted power 5–10 watts (typ.)
– Enables small, water-cooled optical components farther downstream
10
Implementation
First Optics Enclosure 8-ID-A
– Horizontally-deflecting 12-cm-long side bounce mirror• Currently most problematic component in the beamline with
respect to preserving the source• Small size allows “cheap” replacement as optics fabrication
capabilities improve
11
Implementation
Secondary Optics Enclosure – 8-ID-D
– Horizontal, single-bounce ESRF-designed and -built monochromator
• Effectively fixed energy operation: 7.35 keV• New crystal holder to eliminate vacuum-water connection
allowing eventual removal of upstream Be window• Increased stability and brilliance via better cooling and new
connections to 8-ID-E experiment set-ups
PINK BEAM TO I STATION (XPCS)
MONOCHROMATIC BEAM TO E STATION (GISAXS)
Si(111) or Si(220)
PINK BEAM FROM FOE
“E” Si(220)“G” Si(111)
12
Implementation
Experiment Station 8-ID-E
– GISAXS dominates user program
– Large Q XPCS and liquid surface XPCS
• Require additional user support
Courtesy Oleg Shpyrko, UCSD
Large Q XPCS
Liquid Surface XPCS
13
Implementation
Experiment station 8-ID-I
– Transmission XPCS
– Viscous surface XPCS
– SAXS
– CXDI
Brilliance-preserving monochromator*
Measured stability increases Optical contrast doubled per 2003 values
Re-engineered SAXS set-up
*S. Narayanan et al., J. Synchrotron Rad. 15, 12 (2008)
14
Scientific and General User Program
Many recent high-impact XPCS results obtained at 8-ID
O. G. Shpyrko, E. D. Isaacs, J. M. Logan, Yejun Feng, G. Aeppli, R. Jaramillo, H. C. Kim, T. F. Rosenbaum, P. Zschack, M. Sprung, S. Narayanan, and A. R. Sandy; "Direct measurement of antiferromagnetic domain fluctuations," Nature 447, 68
B. Chung, S. Ramakrishnan, R. Bandyopadhyay, D. Liang, C.F. Zukoski, J.L. Harden, R.L. Leheny, "Microscopic Dynamics of Recovery in Sheared Depletion Gels," Phys. Rev. Lett. 96 (22)
F. Livet, F. Bley, F. Ehrburger-Dolle, I. Morfin, E. Geissler, M. Sutton, "X-ray intensity fluctuation spectroscopy by heterodyne detection," J. Synchrotron Rad. 13 (6), 453-458 (2006).
15
Scientific and General User Program
From last 8-ID sector review (9/2006):“…. I was personally well aware of the very positive direction for Sector 8, but it is particularly nice to have it externally recognized, and especially to hear the scientific impact so highly valued. ….”
Murray (Gibson, ALD Director)
Respectable XPCS-specific publication rate – the majority of which are published in high-impact factor (impact factor ≥ 5) journals
0
1
2
3
4
5
6
7
8
9
10
Nu
mb
er2004 2005 2006 2007
Year
8-ID XPCS Publications
Journal publication
High-impact journal publication
16
Scientific and General User Program
80% of beamtime now allocated through the APS program
– Concomitant increase in GU publications
0
1
2
3
4
5
6
7
8
9
10
Nu
mb
er
2004 2005 2006 2007Year
8-ID XPCS Publications
CAT publication
General user publication
For CY 2007, 8-ID XPCS-time allocated/used as follows:
XPCS Experiment Type Allocation
Small-Q Transmission 63%
Small-Q Liquid Surface 3%
Small-Q Viscous Surface 27%
Large-Q 7%
(infrastructure and/or FTE-limited)
(infrastructure and/or FTE-limited)
17
Scientific and General User Program
8-ID regular and semi-regular General Users (GU’s)– Italics indicate new GU’s since 2003-APS XOR Operations
PI Institution PI Institution
Prof. L. Lurio NIU Prof. S. Mochrie Yale
Prof. M. Sutton McGill University Prof. N. Balsara UC-Berkeley
Prof. M. Foster U. Akron Prof. A. Dhinojwala U. Akron
Prof. S. Sinha UC-San Diego Prof. R. Leheny Johns Hopkins
Prof. J. Harden U. of Ottawa Prof. O. Shpyrko UC-San Diego
Dr. J. Lal ANL Prof. S. Chen MIT
Prof. T. Lodge U. Minnesota Prof. M. Mackay Michigan State
Dr. Steve Dierker BNL Prof. K. Ludwig Boston U.
Dr. C. Gutt HASYLAB Prof. W. Burghardt Northwestern
Dr. P. Thiyagarajan ANL Prof. J. Basu Indian Institute of Science
Prof. H. Kim Sogang University (Korea)
Prof. C. Co University of Cincinnati
Prof. C. Zukoski UIUC
18
Scientific and General User Program
For CY2007, XPCS experiment outcomes were roughly as follows:
Outcome Fraction
Completed Successfully 24%
Ongoing – Partially Successful 63%
Unsuccessful – Beamline Problems 3%
Unsuccessful – Sample Radiation Damage 7%
Unsuccessful – Other Sample Issues 3%
Estimate that (partially) successful experiments run, on average, ~ 3–4 cycles at 18 shifts per cycle before “complete”
Current over-subscription rate for 8-ID is ~ 40%
19
Scientific and General User Program
8-ID, via simultaneous experiment station operations, supports nearly a full end-station complement of XPCS experiments as well as supporting several additional unique experiment capabilities (for various reasons)
Technique “End-Station” Allocation
XPCS 70%
GISAXS 70%
“High-end” SAXS 15%
CXDI 15%
Total 170%
CCD
InjectorslitChamber
Scattered x-ray beam
0.5-m-diam injector
CCD
InjectorslitInjectorslitslitChamber
Scattered x-ray beam
0.5-m-diam injector
0.1
1
10
100
Inte
nsity
[cm
-1]
5 6 7 80.01
2 3 4 5 6 7
Q [A-1
]
Experimental Intensity
Model calculated Intensity
4sin/ (Å-1)
0.1
1
10
100
Inte
nsity
[cm
-1]
5 6 7 80.01
2 3 4 5 6 7
Q [A-1
]
Experimental Intensity
Model calculated Intensity
4sin/ (Å-1)
CXDI from de-alloyed AgAu particlePartial reconstruction
(X. Xiao and Q. Shen, ANL)
TR-SAXS from supercritical condensates(S. Lin and C. Carter, WPAFB)
20
Scientific and General User Program
Despite simultaneous station operations, several intimately and peripherally related programs remain under-developed at 8-ID because of lack of:
– Beamtime
– FTE’s
– Infrastructure
Under-developed coherence-related programs at 8-ID include
– Large Q XPCS
– Liquid surface XPCS
– Hard x-ray coherent x-ray diffraction imaging (CXDI)
Transmission small-angle XPCS could grow significantly as well
– Aggressive outreach efforts are limited by the lack of available beamtime
There remains significant room for growth in the field of XPCS!
21
Opportunities for Improvement
Despite ubiquitous XPCS phase diagram to the contrary, XPCS experiments to-date have been restricted to lower left corner of theoretically accessible phase space
*Graphic courtesy of A. Robert, SLAC
*
Access to larger wave-vector transfers and/or higher frequencies requires brighter sources like NSLS-II and better utilization of the coherent flux delivered by 3rd generation sources
22
Opportunities for Improvement
XPCS “tomorrow”XPCS today
Today, in order to remain in the diffraction limit, only 10% of the coherent flux delivered by the undulator is used for 8-ID XPCS experiments
– The vertical coherence length is too large
Brilliance-preserving vertical focusing allows the vertical coherence length to be tailored so that the entire coherent flux can be used
– XPCS signal-to-noise ratio considerations show that 100× faster dynamics or 10× weaker scatterers can be studied
23
Opportunities for Improvement
Vertical focusing at NSLS-II can be effectively implemented via kinoform lenses
Sample
K. Evans-Lutterodt et al., Opt. Express 11, 919 (2003)
Currently examining lens with the following properties:
•Efficiency 50% at 7. 35 keV
•1-σ focal line width = 0.9 m (0.8 m ideal)
•1.04 m focal length (0.97 m ideal)
24
Opportunities for ImprovementQ
y (n
m-1
)27 m × 20 m (V×H)
unfocused200 m × 20 m (V×H)
unfocused200 m × 20 m (V×H)
focused
×1 ×0.1 ×0.2Q x (nm-1 )
25
Opportunities for Improvement
))()(()()(),( 212121 rIrIrIrIrrC
Qy (
nm
-1)
27 m × 20 m (V×H) unfocused
Q x (nm-1 )
200 m × 20 m (V×H) unfocused
200 m × 20 m (V×H) focused
Spatial Autocorrelation:
26
Opportunities for Improvement
End station design needs to be included in the beamline design process
Number and best type of staffing for beamlines needs to be considered carefully
– At APS 3 beamline scientists and 0.5 of a scientific associate support 2 simultaneously operating beamlines at 8-ID
• Many recent GU’s have very little scattering background• Increased staffing is an obvious remedy but serious thought should
be given to the type of staff especially with more specialized “static” beamlines– Operations manager per ESRF– Beamline scientists provide more strategic support and user
recruitment per neutron facilities– Scientific associates– Scientific computing support
27
Challenges
Competition for both quality GU’s and quality beamline staff from nascent 3rd and 4th generation XPCS facilities and existing 3rd generation facilities
– SLS, Diamond, Petra-III• Enhanced brightness and/or sophisticated
detector programs
– LCLS and XFEL• Different kettle of fish
– APS and ESRF• Fully operational with significant upgrade
plans/possibilities
Detectors!
– Powerful detectors are needed to effectively utilize increased coherent flux
28
8-ID Help Wanted